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Tricritical points in the Sherrington-Kirkpatrick model in the presence of discrete random fields

机译:存在离散随机场的Sherrington-Kirkpatrick模型中的三临界点

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The infinite-range-interaction Ising spin glass is considered in the presence of an external random magnetic field following a trimodal (three-peak) distribution. Such a distribution corresponds to a bimodal added to a probability po for a field dilution, in such a way that at each site the field h(i) obeys P(h(i))=p+delta(h(i)-h(0)) +p(0)delta(h(i))+p(-)delta(h(i)+h(0)). The model is studied through the replica method and phase diagrams are obtained within the replica-symmetry approximation. It is shown that the border of the ferromagnetic phase may present, for conveniently chosen values of p(0) and h(0), first-order phase transitions, as well as tricritical points at finite temperatures. Analogous to what happens for the Ising ferromagnet under a trimodal random field, it is verified that the first-order phase transitions are directly related to the dilution in the fields: the extensions of these transitions are reduced for increasing values of p(0). Whenever the delta function at the origin becomes comparable to those at h(i)=+/-h(0), first-order phase transitions disappear; in fact, the threshold value p(0)*, above which all phase transitions are continuous, is calculated analytically as p(0)*=2(e(3/2)+2)(-1)approximate to 0.30856. The ferromagnetic boundary at zero temperature also exhibits an interesting behavior: for 0(0)(0)*, a single tricritical point occurs, whereas if p(0)>p(0)* the critical frontier is completely continuous; however, far p(0)=p(0)*, a fourth-order critical point appears. Stability analysis of the replica-symmetric solution is performed and the regions of validity of such a solution are identified; in particular, the Almeida-Thouless line in the plane field versus temperature is shown to depend on the weight p(0). [References: 64]
机译:在存在遵循三峰(三峰)分布的外部随机磁场的情况下,考虑了无限范围相互作用的Ising自旋玻璃。这样的分布对应于添加到场稀释概率po上的双峰分布,以这种方式使得场h(i)服从P(h(i))= p + delta(h(i)-h (0))+ p(0)delta(h(i))+ p(-)delta(h(i)+ h(0))。通过复制方法研究模型,并在复制对称近似内获得相位图。结果表明,对于方便选择的p(0)和h(0)值,铁磁相的边界可能存在一阶相变以及有限温度下的三临界点。类似于在三峰随机场下对Ising铁磁体所发生的情况,已证实一阶相变与场中的稀释直接相关:这些跃迁的扩展随着p(0)值的增加而减小。每当原点处的增量函数与h(i)= + /-h(0)处的增量函数具有可比性时,一阶相变就会消失;实际上,所有相变都连续的阈值p(0)*解析为p(0)* = 2(e(3/2)+2)(-1)近似为0.30856。零温度下的铁磁边界也表现出有趣的行为:对于0 (0)(0)*,会出现单个三临界点,而如果p(0)> p(0)*,则临界边界是完全连续的;但是,远p(0)= p(0)*,出现了四阶临界点。进行复制对称解决方案的稳定性分析,并确定这种解决方案的有效性区域;尤其是,平面场中的Almeida-Thouless线与温度的关系曲线取决于重量p(0)。 [参考:64]

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